Measurement of the distributions of event-by-event flow harmonics in lead-lead collisions at √s[subscript NN] = 2.76 TeV with the ATLAS detector at the LHC
The distributions of event-by-event harmonic flow coefficients v [subscript n] for n = 2- 4 are measured in √s[subscript NN] = 2.76 TeV Pb + Pb collisions using the ATLAS detector at the LHC. The measurements are performed using charged particles with transverse momentum p [subscript T] > 0.5 GeV...
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| Format: | Article |
| Language: | en_US |
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Springer-Verlag
2014
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| Online Access: | http://hdl.handle.net/1721.1/86023 https://orcid.org/0000-0002-7586-7253 |
| Summary: | The distributions of event-by-event harmonic flow coefficients v [subscript n] for n = 2- 4 are measured in √s[subscript NN] = 2.76 TeV Pb + Pb collisions using the ATLAS detector at the LHC. The measurements are performed using charged particles with transverse momentum p [subscript T] > 0.5 GeV and in the pseudorapidity range |η| < 2.5 in a dataset of approximately 7 μb[superscript −1] recorded in 2010. The shapes of the v [subscript n] distributions suggest that the associated flow vectors are described by a two-dimensional Gaussian function in central collisions for v [subscript 2] and over most of the measured centrality range for v [subscript 3] and v [subscript 4]. Significant deviations from this function are observed for v [subscript 2] in mid-central and peripheral collisions, and a small deviation is observed for v [subscript 3] in mid-central collisions. In order to be sensitive to these deviations, it is shown that the commonly used multi-particle cumulants, involving four particles or more, need to be measured with a precision better than a few percent. The v [subscript n] distributions are also measured independently for charged particles with 0.5 < p [subscript T] < 1 GeV and p [subscript T] > 1 GeV. When these distributions are rescaled to the same mean values, the adjusted shapes are found to be nearly the same for these two p [subscript T] ranges. The v [subscript n] distributions are compared with the eccentricity distributions from two models for the initial collision geometry: a Glauber model and a model that includes corrections to the initial geometry due to gluon saturation effects. Both models fail to describe the experimental data consistently over most of the measured centrality range. |
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